ebook img

Polymer films characterized by Positron Annihilation Spectroscopy PDF

19 Pages·2002·0.28 MB·English
by  
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview Polymer films characterized by Positron Annihilation Spectroscopy

Sm(cid:142) inaire LAPP , 11 octobre 2002 Polymer films characterized by Positron Annihilation Spectroscopy C. Bas, E. Pinel, S. Neyertz, R. Mercier, N.D. Alb(cid:142) rola Laboratoire Matr(cid:142) iaux Organiques (cid:136) Proprit(cid:142) s(cid:142) Sp (cid:142) cifiques (LMOPS) - UMR 5041 M.-F. Barthe, P. Desgardin Centre d’Etudes et de Recherches par Irradiation (CERI) - UPR33 1 Background In a polymer, different types of positrons : Positron-Electron pair (e+,e-) Free Positron (e+) Positronium Ps pPs oPs Annihilation Intrinsic Annihilation Pick-off Annihilation g g g g g g e++ e- (cid:25) 2 g Lifetime t = 0.125 ns 1 Lifetime t = 0.4 ns 2 Lifetime t > 0.5 ns 3 Intrinsic annihilation g Lifetime t = " In vacuum g 2 g Lifetime t = 142 ns 3 2 t and t are constant 1 2 t depends on the polymer microstructure 3 Electron cloud - 1 Ø R 1 (cid:230) 2¶ (cid:215) R (cid:246) ø (cid:153) = 0.5(cid:215) Œ 1- + sin(cid:231) (cid:247) œ 3 º R + D R 2¶ Ł R + D R ł ß oPs 2.2 (cid:129) R D R D R : electron layer thickness around the hole = 1.66 (cid:129) Bulk polymer Tao-Eldrup model [*] => detection of holes with diameter ranged from 3 (cid:129) to 15 (cid:129) [*] J. Chem. Phys.(1972) 56, 5499 3 Chem. Phys. (1981) 63, 51 Birth g -ray Background qqqq 1.27 MeV DDDD t = tttt g -ray annihilation E = 0.511 MeV – DDDD E Sample Na22 (cid:25) Ne22 + e+ + g Positron source 22Na Diffusion (100nm) g -ray annihilation E = 0.511 MeV – DDDD E Thermalization (1ps) (cid:255) Measurement of positron lifetime DDDD t = tttt (Positron Annihilation Lifetime Spectroscopy - PALS) (cid:255) Measurement of energy broadening DDDD E = p c/2 z (Doppler Broadenning Spectrocopy - DBS) (cid:255) qqqq Measurement of angle (Angular Correlation of Annihilation Radiation - ACAR) 4 Apparatus (cid:255) Measurement of positron lifetime DDDD t = tttt (Positron Annihilation Lifetime Spectroscopy - PALS) Example of spectrum PMT : Photomultiplicateur CFDD : Constant fraction differential discriminator From this spectrum, it is possible to determine : TAC : Time to amplitude converter I , t (cid:247) pPs ADC : Analogue-to-digital converter 1 1 I , t (cid:247) e+ 2 2 MAC : mulitchannel analyzer I , t (cid:247) oPs 3 3 5 Background Origin of energy broadening DDDD E : (cid:255) is related to the bound energy of the annihilation electron (or momentum e +,e- pair) ¨ if the free positron annihilates with a valence electron, D E is low ¨ if the free positron annihilates with a core electron, D E is high => broadening effect Positron-Electron pair (e+,e-) Free Positron (e+) Positronium Ps pPs oPs Annihilation Instrinsic Annihilation Pick-off Annihilation g g g g g g e++ e- (cid:25) 2 g Narrow Doppler line Broad Doppler line Broad Doppler line 6 DBS peak S parameter: S = As / At ˛ S mainly related to annihilations with valence electrons ˛ structural informations (defects) s As t n u o W parameter: C W = Aw / At Aw Aw ˛ W mainly related to annihilations with core electrons ˛ Chemical informations 504 506 508 510 512 514 516 518 Energy (keV) S-parameter W-parameter 0,59 0,20 0,58 0,19 0,57 0,18 0,56 0,17 32 34 36 38 40 42 44 7 oPs intensity - I (%) 3 Slow positron beam Positron source of 22Na : maximum of energy of 540Kev The mean implantation depth of the positrons ( z ) depends on the incident positron energy (E) o 400 z(A) = . E(keV)1.6 d For polymer with d =1.3 : 540 keV · 700 m m 25 keV · 5 m m Cao et al. Appl. Surf. Sci. (1999), 149, 116 8 French positron facility for materials science Strasbourg Ires --- Arcueil PALS DGA - ? --- --- milieux micellaires 1 chercheur ---- 1 chercheur Chambr(cid:142) y / Annecy LMOPS / LAPP --- Orla(cid:142) ns PALS (fin 2002) CERI --- --- No slow positron pulsing system matr(cid:142) iaux peu Positron beam coupled with denses DBS + PALS with 22Na source --- Semi-conducteurs ---- 2 chercheurs 9 Our results CERI facility : positron beam with positron energy from 0.5 keV to 25 keV coupled with DBS Preliminary results with PALS from Perkin Elmer (to be confirmed) Samples : films of 20 to 30 m m thickness polyimides O ODA-CF3 O ODOPA O O BCDA O C(CH ) O C(CH ) 33 33 N O N N O N N O N x y n O CF O O CF O O CF O 3 3 3 Mean depth (m m) 0 0.4 1.2 2.3 3.6 5.2 0.47 0.050 BCDA-ODA O O 0.048 N N O r e r t 0.46 e O O e t m 0.046 e m a r a a r p 0.044 a - p S 0.45 - W 0.042 0.44 0.040 0 5 10 15 20 25 10 Energy (keV)

Description:
by Positron Annihilation Spectroscopy. C. Bas, E. Pinel, S. Neyertz, R. Mercier, N.D. Alb rola. Laboratoire Matriaux Organiques Proprit s Sp cifiques (LMOPS)
See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.